Moving on, we transform and remove this second type of operators including \(\partial ^2 h\)  that are generated in SMEFT; we will make use of the EoM of the Higgs field, which causes a difference that is pushed to higher orders in the expansion that are not included anyway, so that at fixed order they are equivalent. The EoM (within the electroweak sector alone) reads [1]}, [2]}, [3]}, [4]}
\(\partial ^2h&=& \frac{(v+h)}{2}\,\langle D_\mu U^\dagger D^\mu U\rangle \, -\, V^{\prime }(h)\, ,\) 
